Development of high poloidal beta, steady-state scenario with ITER-like tungsten divertor on EAST
文献类型:期刊论文
作者 | Garofalo, A. M.1; Gong, X. Z.2; Qian, J.2; Chen, J.2; Li, G.2; Li, K.2; Li, M. H.2; Zhai, X.2; Bonoli, P.3; Brower, D.4 |
刊名 | NUCLEAR FUSION |
出版日期 | 2017-07-01 |
卷号 | 57期号:7页码:1-9 |
关键词 | Magnetic Fusion Steady-state Tokamak Current Profile Control Lower Hybrid |
DOI | 10.1088/1741-4326/aa7186 |
文献子类 | Article |
英文摘要 | Recent experiments on EAST have achieved the first long pulse H-mode (61 s) with zero loop voltage and an ITER-like tungsten divertor, and have demonstrated access to broad plasma current profiles by increasing the density in fully-noninductive lower hybrid current-driven discharges. These long pulse discharges reach wall thermal and particle balance, exhibit stationary good confinement (H-98y2 similar to 1.1) with low core electron transport, and are only possible with optimal active cooling of the tungsten armors. In separate experiments, the electron density was systematically varied in order to study its effect on the deposition profile of the external lower hybrid current drive (LHCD), while keeping the plasma in fully-noninductive conditions and with divertor strike points on the tungsten divertor. A broadening of the current profile is found, as indicated by lower values of the internal inductance at higher density. A broad current profile is attractive because, among other reasons, it enables internal transport barriers at large minor radius, leading to improved confinement as shown in companion DIII-D experiments. These experiments strengthen the physics basis for achieving high performance, steady state discharges in future burning plasmas. |
WOS关键词 | NUCLEAR-SCIENCE FACILITY ; TRANSPORT ; TOKAMAK ; JET |
WOS研究方向 | Physics |
语种 | 英语 |
WOS记录号 | WOS:000403320400001 |
资助机构 | US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; US Department of Energy, Office of Science, Office of Fusion Energy Sciences(DE-FC02-04ER54698 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; National Magnetic Confinement Fusion Program of China(2015GB102002 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; DE-SC0010685 ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; 2015GB103000) ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-SC-0010492 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-FG02-01ER54615 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC02-09CH11466 ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) ; DE-AC52-07NA27344) |
源URL | [http://ir.hfcas.ac.cn:8080/handle/334002/31875] |
专题 | 合肥物质科学研究院_中科院等离子体物理研究所 |
作者单位 | 1.Gen Atom, San Diego, CA 92186 USA 2.Chinese Acad Sci, Inst Plasma Phys, Hefei 230031, Anhui, Peoples R China 3.MIT, Plasma Sci & Fus Ctr, 77 Massachusetts Ave, Cambridge, MA 02139 USA 4.Univ Calif Los Angeles, Dept Phys & Astron, Los Angeles, CA 90095 USA 5.Princeton Plasma Phys Lab, POB 451, Princeton, NJ 08543 USA 6.Lawrence Livermore Natl Lab, Livermore, CA 94551 USA 7.Oak Ridge Associated Univ, Oak Ridge, TN 37830 USA 8.CEA, IRFM, F-13108 St Paul Les Durance, France |
推荐引用方式 GB/T 7714 | Garofalo, A. M.,Gong, X. Z.,Qian, J.,et al. Development of high poloidal beta, steady-state scenario with ITER-like tungsten divertor on EAST[J]. NUCLEAR FUSION,2017,57(7):1-9. |
APA | Garofalo, A. M..,Gong, X. Z..,Qian, J..,Chen, J..,Li, G..,...&Wan, B..(2017).Development of high poloidal beta, steady-state scenario with ITER-like tungsten divertor on EAST.NUCLEAR FUSION,57(7),1-9. |
MLA | Garofalo, A. M.,et al."Development of high poloidal beta, steady-state scenario with ITER-like tungsten divertor on EAST".NUCLEAR FUSION 57.7(2017):1-9. |
入库方式: OAI收割
来源:合肥物质科学研究院
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